JPS5937658B2 - Method for improving iron loss in stators of large rotating electric machines - Google Patents
Method for improving iron loss in stators of large rotating electric machinesInfo
- Publication number
- JPS5937658B2 JPS5937658B2 JP54160502A JP16050279A JPS5937658B2 JP S5937658 B2 JPS5937658 B2 JP S5937658B2 JP 54160502 A JP54160502 A JP 54160502A JP 16050279 A JP16050279 A JP 16050279A JP S5937658 B2 JPS5937658 B2 JP S5937658B2
- Authority
- JP
- Japan
- Prior art keywords
- laser beam
- iron loss
- rolling
- fan
- rotating electric
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K15/00—Processes or apparatus specially adapted for manufacturing, assembling, maintaining or repairing of dynamo-electric machines
- H02K15/02—Processes or apparatus specially adapted for manufacturing, assembling, maintaining or repairing of dynamo-electric machines of stator or rotor bodies
- H02K15/021—Magnetic cores
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B23—MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K2103/00—Materials to be soldered, welded or cut
- B23K2103/02—Iron or ferrous alloys
- B23K2103/04—Steel or steel alloys
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K2201/00—Specific aspects not provided for in the other groups of this subclass relating to the magnetic circuits
- H02K2201/06—Magnetic cores, or permanent magnets characterised by their skew
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Power Engineering (AREA)
- Manufacture Of Motors, Generators (AREA)
Description
【発明の詳細な説明】
本発明は、一方向性電磁鋼板を使用した大型回転電機固
定子の鉄損改善方法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for improving iron loss in a stator of a large rotating electric machine using a unidirectional electrical steel sheet.
磁気特性に優れた電磁鋼板には一方向性電磁鋼板がある
が、これは圧延方向に(001,1軸が向き(110)
面が圧延面に平行になるようにしたもので、圧延方向つ
まり鋼板ストリップの長さ方向には磁化は容易であるが
、幅方向は(110)軸になるので磁化は容易でない。Unidirectional electrical steel sheets are examples of electrical steel sheets with excellent magnetic properties;
The surface is parallel to the rolling surface, and magnetization is easy in the rolling direction, that is, the length direction of the steel strip, but it is not easy to magnetize in the width direction because it is the (110) axis.
電動機2発電機などの回転電機の固定子および回転子は
一般に積層鉄心を使用し、所定形状の各鉄心素子を鋼板
から打抜き、それを所定厚みに積み重ね、結束してなる
が、各鉄心素子は回転子なら外周面に多数の歯部を持つ
円環状、固定子なら内周面に多数の歯部を持つ円環状で
あり、磁束は歯部で放射方向(半径方向)、継鉄部で円
周方向に通る。The stator and rotor of rotating electric machines such as electric motors and generators generally use a laminated core, and each core element of a predetermined shape is punched out of a steel plate, stacked to a predetermined thickness, and bundled. The rotor has a circular shape with many teeth on the outer circumferential surface, and the stator has a circular shape with many teeth on the inner circumferential surface.The magnetic flux flows in the radial direction (radial direction) at the teeth and in the circular direction at the yoke. Passes in the circumferential direction.
つまり磁束は一方向ではなく、360°に亘る任意の方
向に通ることになるので、回転機鉄心に方向性電磁鋼板
を適用するには難があり、従来これには無方向電磁鋼板
を使用するのが普通であった。In other words, the magnetic flux does not pass in one direction, but in any direction over 360°, which makes it difficult to use grain-oriented electrical steel sheets for rotating machine cores. Conventionally, non-oriented electrical steel sheets have been used for this purpose. It was common.
しかし大型回転機は、その環状固定子鉄心素子を鋼板か
ら直接打抜くには寸法が大き過ぎるので複数個に分割し
てその扇形鉄心素子を鋼板から打抜き、それを集めて円
環状としかつ所定厚みの固定子に積層する。However, for large rotating machines, the size of the annular stator core element is too large to be punched directly from a steel plate, so the fan-shaped core element is divided into multiple parts and then punched out from the steel plate. Laminated on the stator.
この場合は扇形鉄心素子の継鉄部または歯部を圧延方向
にはゾ合せることが可能で風るので、一方向性電磁鋼板
の使用が可能であり、実際に使用されてもいる。In this case, the yoke or teeth of the fan-shaped core element can be aligned in the rolling direction, so unidirectional electrical steel sheets can be used, and are actually used.
しか(7この場合も継鉄部を圧延方向に合せれば歯部で
は磁束方向は(110)軸方向となり、歯部を圧延力向
にとれば継鉄部の磁束方向が〔110〕軸力向になり、
いずれにしても不都合が生じる。However, (7) In this case as well, if the yoke section is aligned with the rolling direction, the magnetic flux direction at the tooth section will be the (110) axial direction, and if the tooth section is aligned with the rolling force direction, the magnetic flux direction at the yoke section will be the [110] axial force. Turning towards
In either case, inconvenience will occur.
か5る問題は冶金学的に解決することが本節ではあり5
2方向性電磁鋼板なども開発されているが、これはまた
低コストで量産化可能な状態にはない。This section aims to solve these problems metallurgically.
Although bidirectional electrical steel sheets and the like have been developed, they are not in a state where they can be mass-produced at low cost.
本発明はいわば物理的な方法でこの問題を改善しようと
するものであり、次に図面を参照しながら詳細に説明す
る。The present invention attempts to improve this problem by a so-called physical method, and will be described in detail below with reference to the drawings.
前述のように一方向性電磁鋼板は(110)(001)
組織を持ち、圧延方向に磁化が容易である。As mentioned above, the unidirectional electrical steel sheet is (110) (001)
It has a structure and is easily magnetized in the rolling direction.
か5る鋼板10に対し第1図aに示すように圧延方向F
にほぼ直角にパルスレーザ光を線状、鎖線状または点線
状等の線列状に照射すると(12は線状照射の場合の照
射部分を示す)鉄損が小になる。The rolling direction F is as shown in FIG.
When pulsed laser light is irradiated in a linear array such as a line, a chain line, or a dotted line substantially perpendicular to the line (12 indicates the irradiated portion in the case of linear irradiation), iron loss is reduced.
これは次のように説明できる。即ち一方向性電磁鋼板1
0は第2図aに示すように圧延方向に延びる比較的大き
な磁区14を有する。This can be explained as follows. That is, unidirectional electrical steel sheet 1
0 has a relatively large magnetic domain 14 extending in the rolling direction, as shown in FIG. 2a.
一方向性電磁鋼板においては(110)[:001)力
位の圧延方向への集積度を高めるにつれて結晶数が大き
くなり、また磁壁が粒界を貫通するために磁区は大きく
なり、磁区の大きさと鉄損値とは比例関係にあるので、
方向性を高めた割り合いには鉄損は少なくならないとい
う矛盾した問題があるものである。In grain-oriented electrical steel sheets, the number of crystals increases as the degree of concentration of (110)[:001) force potential in the rolling direction increases, and the magnetic domain becomes larger because the domain wall penetrates the grain boundary. Since there is a proportional relationship between iron loss and iron loss value,
There is a paradoxical problem in that the iron loss does not decrease as the directionality increases.
これに対し、レーザ光を圧延力向とほぼ直角な方向に照
射すると、その照射部分12の両側に小突起群16が発
生する。On the other hand, when the laser beam is irradiated in a direction substantially perpendicular to the rolling force direction, small protrusions 16 are generated on both sides of the irradiated portion 12.
これは走査型電子顕微鏡等で観察できる。This can be observed using a scanning electron microscope or the like.
なお図では簡単化のため小突起は一部しか示していない
。Note that in the figure, only a portion of the small protrusions are shown for simplicity.
この小突起は磁区(マグネチックドメイン)の芽であっ
て、磁化されるとき鋼板10の磁区14はこの芽から伸
びる磁区18により細分化される。These small protrusions are buds of magnetic domains, and when magnetized, the magnetic domains 14 of the steel sheet 10 are subdivided by magnetic domains 18 extending from these buds.
従って鉄損は小になる。Therefore, iron loss becomes small.
小突起群16が生じるのは、鋼板10にパルスレーザを
照射すると転位が発生し、磁区の芽の発生確率はこの転
位の密度に比例することに依ると考えられる。It is thought that the small protrusions 16 are generated because dislocations occur when the steel plate 10 is irradiated with a pulsed laser, and the probability of occurrence of magnetic domain buds is proportional to the density of these dislocations.
第1図すに示すようにレーザ光を圧延方向に照射すると
、第2図すに示すようにやはり小突起群16が発生する
。When the laser beam is irradiated in the rolling direction as shown in FIG. 1, small protrusions 16 are also generated as shown in FIG. 2.
外部磁界Hが作用するときこの芽16より微小ドメイン
が発生し鉄損を下げるものと考えられる。It is thought that when an external magnetic field H acts, microdomains are generated from this bud 16, which lowers the iron loss.
具体例を挙げると第1図aのようにレーザ光照射したも
のの圧延力向の鉄損WL(磁束密度1.7T、周波数5
0Hz)は]、、 00 W/kgとなり、圧延力向と
直角方向の鉄損Wc(磁束密度1.3T、周波数50H
z)はレーザ光照射しないものと殆んど同じである。To give a specific example, as shown in Figure 1a, the iron loss WL in the rolling force direction (magnetic flux density 1.7T, frequency 5
0Hz) is ],, 00 W/kg, and the iron loss Wc in the direction perpendicular to the rolling force direction (magnetic flux density 1.3T, frequency 50H
z) is almost the same as that without laser beam irradiation.
なお、レーザ光照射前のもののwLは1.10 ’W/
kg、Wcは2.84W/kgである。In addition, wL before laser beam irradiation is 1.10'W/
kg, Wc is 2.84W/kg.
つまり第1図aのレーザ光照射で10%のWLの減少が
可能になる。In other words, the laser beam irradiation shown in FIG. 1a allows a 10% reduction in WL.
第1図すの場合はWLは殆んど変らず、Wcは2.04
W/kgとなり、約28%と大幅なWcの減少が可能
となった。In the case of Figure 1, WL hardly changes and Wc is 2.04.
W/kg, making it possible to significantly reduce Wc by approximately 28%.
このような効果を得るには、レーザ光照射に条件があい
、先ずレーザ光照射部分12の幅dとピッチlであるが
、第1図aの場合はd二0.01〜1、mm、1に1〜
20m7rL1 レーザパルスの時間幅は1 nS−
100msがよい。In order to obtain such an effect, conditions are met for laser beam irradiation, first of all, the width d and pitch l of the laser beam irradiated portion 12, in the case of FIG. 1 to 1~
20m7rL1 The time width of the laser pulse is 1 nS-
100ms is good.
エネルギ密度Pは0.01〜1oooJ、/=が好まし
い。The energy density P is preferably 0.01 to 1oooJ, /=.
なお、パルスレーザ光を照射する場合、照射部分が鎖線
状または点線状に配列されるときには、第1図aにおい
てはL方向直径d=0.01〜1mm、照射点C方向間
隔aは3rIL1rL以下、好ましくは1mrn以下が
よい。In addition, when irradiating pulsed laser light, when the irradiated parts are arranged in a chain line or dotted line, the diameter d in the L direction is 0.01 to 1 mm in FIG. , preferably 1 mrn or less.
また第1図すではC方向直径d=0.01〜11111
1L、照射点し方向間隔aは3r/lT/L以下、好ま
しくはLmvt以下にすることが必要である。Also, in Figure 1, the diameter in the C direction d = 0.01 to 11111
1L, the directional spacing a between the irradiation points must be 3r/lT/L or less, preferably Lmvt or less.
第1図a、t)共レーザ光照射部分12の向きはそれぞ
れ正確に圧延力向に直角および平行整列していなくても
、それよりも±30°程度の範囲でずれる分には効果に
は格別の差はない。Fig. 1 a, t) Even if the direction of the co-laser beam irradiation portion 12 is not aligned at right angles and parallel to the direction of rolling force, it will not be effective as long as it deviates within a range of ±30°. There is no particular difference.
そこで本発明では分割固定子構造の大型回転機固定鉄心
を構成する鋼板素子に上述のレーザ光照射を行ない、磁
束がほぼ圧延力向と直角な方向に通る部分でその鉄損を
減少させまた磁束が圧延方向に通る部分でもその鉄損を
更に減少させようとするものである。Therefore, in the present invention, the steel plate elements constituting the fixed core of a large rotating machine with a split stator structure are irradiated with the above-mentioned laser beam to reduce the iron loss in the portion where the magnetic flux passes in a direction approximately perpendicular to the rolling force direction. The aim is to further reduce the iron loss in the portion where the iron passes in the rolling direction.
第3図aは一方向性電磁鋼板(圧延方向はF)10から
固定子鉄心を打抜く要領を示し、20は扇形の固定子鉄
心素子であり、20bはその歯部、20aは継鉄部であ
る。Figure 3a shows the procedure for punching a stator core from a unidirectional electrical steel sheet (rolling direction is F) 10, 20 is a fan-shaped stator core element, 20b is a tooth thereof, and 20a is a yoke. It is.
一方向性電磁鋼板10の幅Wは1m程度であり、かXる
鋼板10から無駄少なく鉄心素子20を採取するため、
隣合う鉄心素子20’ 、 20//は逆向きにしたり
する。The width W of the unidirectional electrical steel sheet 10 is about 1 m, and in order to extract the iron core element 20 from the steel sheet 10 with less waste,
Adjacent core elements 20', 20// may be oriented in opposite directions.
鉄心素子20の長手方向F1は鋼板10の圧延力向Fに
合せる。The longitudinal direction F1 of the iron core element 20 is aligned with the rolling force direction F of the steel plate 10.
こ5で、長手方向F1とは、扇形素子20の中心におけ
る半径方向R1と直交する方向であるとする。Here, it is assumed that the longitudinal direction F1 is a direction perpendicular to the radial direction R1 at the center of the fan-shaped element 20.
鉄心素子中の磁束は第3図すに点線で示すように継鉄部
では円周方向F2、歯部では半径方向、継鉄部と歯部と
の境界部ではこれらをつなぐ弧状(これは例えば3相励
磁するなら各時点の電流位相で左側または右側へ曲る弧
状)となる。As shown by the dotted line in Figure 3, the magnetic flux in the core element is in the circumferential direction F2 at the yoke, in the radial direction at the tooth, and in the arc shape connecting these at the boundary between the yoke and the tooth. If three-phase excitation is used, it will be an arc shape that bends to the left or right depending on the current phase at each point in time.
そこで継鉄部に関しては扇形素子20の中心で磁束方向
を圧延力向に合せれば、左、右端では磁束方向(本来の
)は圧延力向つまり磁化容易なCool)軸力向からず
れ、このずれの角度は固定子の分割数によって変るが通
常20〜30°になる。Therefore, regarding the yoke part, if the magnetic flux direction is aligned with the rolling force direction at the center of the fan-shaped element 20, the magnetic flux direction (original) at the left and right ends will deviate from the rolling force direction, that is, the direction of the easy-to-magnetize (Cool) axial force, and this The angle of deviation varies depending on the number of divisions of the stator, but is usually 20 to 30 degrees.
また歯部20bにおいては、扇形素子長手方向F1を圧
延力向Fに合せれば、扇形素子中心の歯部の磁束方向は
圧延力向と直交する方向となり、扇形素子左、右端部で
はそれより20〜30°ずれることになる。In addition, in the tooth portion 20b, if the longitudinal direction F1 of the fan-shaped element is aligned with the rolling force direction F, the magnetic flux direction of the tooth portion at the center of the fan-shaped element becomes a direction perpendicular to the rolling force direction, and the magnetic flux direction at the left and right end portions of the fan-shaped element is It will be shifted by 20 to 30 degrees.
一方向性電磁鋼板では(110)[’0O1)組織の圧
延方向への集積度を高めることが大幅な鉄損改善を達成
し得たことからも分るように、磁区方向と磁束方向のず
れは鉄損に大きな影響を与えるから、この20〜30°
のずれも無視できない問題である。In unidirectional electrical steel sheets, increasing the degree of integration of the (110) ['0O1) structure in the rolling direction can significantly improve iron loss. This 20~30° has a great effect on iron loss.
The misalignment is also a problem that cannot be ignored.
まして歯部においては磁束は〔001〕軸と直交〔11
0〕軸つまり磁化は容易でない方向に通り、更に歯部と
継鉄部との境界部では磁化困難な(111)方向に通る
ことにもなり、これは一方向性電磁鋼板の回転機への適
用を断念させる理由となる。Moreover, in the teeth, the magnetic flux is perpendicular to the [001] axis [11
0] Axis, that is, magnetization passes in a direction that is difficult, and furthermore, at the boundary between the teeth and the yoke, magnetization passes in the (111) direction, which is difficult to achieve. This is a reason to give up on application.
そこで本発明では一方向性電磁鋼板から上記のように方
向を合せて打抜いた扇形固定鉄心素子20に対して第3
図すの縞模様の如くパルスレーザ光照射を行なう。Therefore, in the present invention, a third
Pulsed laser light is irradiated as shown in the striped pattern shown in the figure.
即ち素子20の継鉄部20aに対しては第1図aの方法
を採って、所定幅dのレーザ光照射部分12がC方向(
半径方向)に延びかつ所定間隔lをピッチとしてL方向
(円周方向)に並ぶようにレーザ光を照射し、歯部20
bでは第1図すの方法を採って所定幅dのレーザ光照射
部分12がL方向(円周方向〕に延びかつ所定間隔lを
ピッチとし、てC方向(半径方向)に並ぶようにする。That is, for the yoke part 20a of the element 20, the method shown in FIG.
The teeth 20 are irradiated with laser light so as to extend in the L direction (radial direction) and line up in the L direction (circumferential direction) with a pitch of a predetermined interval l.
In b, by adopting the method shown in Fig. 1, the laser beam irradiated portions 12 of a predetermined width d extend in the L direction (circumferential direction) and are lined up in the C direction (radial direction) with a pitch of a predetermined interval l. .
レーザ光照射部分12を作るにはパルスレーザ光を逐次
偏向するつまり走査してもよく、またはスリットなどで
制限して部分12に一致する細帯状のパルスレーザ光を
照射してもよい。In order to create the laser beam irradiation portion 12, the pulsed laser beam may be sequentially deflected, that is, scanned, or the pulsed laser beam may be limited by a slit or the like and a narrow strip of pulsed laser beam that coincides with the portion 12 may be irradiated.
この後者のパターン照射の場合は更に複数個のレーザ光
照射部分12を同時に投射するようにしてもよい。In the case of the latter pattern irradiation, a plurality of laser beam irradiation portions 12 may be projected simultaneously.
歯部20bのレーザ光照射部分12は弧状とする代りに
直線としても両者のずれは僅小である。Even if the laser beam irradiated portion 12 of the tooth portion 20b is formed into a straight line instead of an arc, the deviation between the two is very small.
第1図a、bの方法をこの鉄心素子20にそのま5適用
すると、継鉄部20aではレーザ光照射部分12はすべ
てその中心における半径R1に平行な方向に延びること
になり、扇形端部では上記とは20〜30°のずれを生
じる。If the methods shown in FIGS. 1a and 1b are directly applied to this core element 20, all of the laser beam irradiated parts 12 in the yoke part 20a will extend in a direction parallel to the radius R1 at the center, and the fan-shaped end Then, a deviation of 20 to 30 degrees occurs from the above.
また、歯部20bでも同様で、扇形素子20の中心の半
径R1に直角な方向つまり前述の長手方向F1にすべて
平行にレーザ光照射部分12は延びることになり、扇形
端部では上記とは20〜30°のずれを生じる。The same applies to the tooth portion 20b, and the laser beam irradiation portion 12 extends in a direction perpendicular to the radius R1 of the center of the fan-shaped element 20, that is, in parallel to the aforementioned longitudinal direction F1. This results in a deviation of ~30°.
しかしこの程度のずれは前述の理由で許容でき、しかも
このずれ1電磁束の方向に適合するものであるからむし
ろ好ましい効果を期待できる。However, this degree of deviation is permissible for the reasons mentioned above, and since this deviation corresponds to the direction of one electromagnetic flux, a rather favorable effect can be expected.
歯部20bと継鉄部20aとの境界部に対しては、図示
の如く歯部20bに対するレーザ光照射要領を先細り状
に適用すると磁束は鎖線方向に案内され、第1図a、b
で説明した理由により鉄損の減少を図ることができるが
、この部分は第3図Cに示すように継鉄部のレーザ光照
射要領を適用してもよく、また磁束が種々の方向を向き
そして量的には少ないので第3図dのようにレーザ照射
しないことにしてもよい。If the laser beam irradiation method for the tooth portion 20b is applied in a tapered manner to the boundary between the tooth portion 20b and the yoke portion 20a as shown in the figure, the magnetic flux is guided in the direction of the chain line, and as shown in FIGS.
The iron loss can be reduced for the reason explained in 2. However, the laser beam irradiation procedure for the yoke part as shown in Fig. 3C may be applied to this part, and the magnetic flux may be oriented in various directions. Since the quantity is small, it may be decided not to irradiate the laser as shown in FIG. 3d.
以上説明1−たように本発明によれば一方向性電磁鋼板
使用の分割固定子型回転電機の固定子鉄損を歯部および
継鉄部ともに改善することができる。As explained above, according to the present invention, it is possible to improve the stator core loss in both the tooth portion and the yoke portion of a split stator type rotating electrical machine using unidirectional electrical steel sheets.
周知のように鉄損は電気機器の稼動中常時発生し、そし
て大型回転電機は長時間連続運転するものが多いので鉄
損減少によるエネルギ節減効果は極めて大きい。As is well known, iron loss occurs constantly during the operation of electrical equipment, and many large rotating electric machines operate continuously for long periods of time, so the energy saving effect of reducing iron loss is extremely large.
第1図a、bはレーザ光照射要領を説明する図、第2図
a+bは鉄損改善理由の説明図、第3図a〜dは本発明
の詳細な説明図である。
図面で、20は分割型固定子鉄心の扇形素子、10は一
方向性硅素鋼板、20aは継鉄部、20bは歯部、12
はレーザ光照射部分である。1A and 1B are diagrams for explaining the procedure of laser beam irradiation, FIGS. 2A and 2B are diagrams for explaining the reason for improving iron loss, and FIGS. 3A to 3D are diagrams for explaining the present invention in detail. In the drawing, 20 is a sector-shaped element of a split stator core, 10 is a unidirectional silicon steel plate, 20a is a yoke part, 20b is a tooth part, 12
is the part irradiated with laser light.
Claims (1)
性電磁鋼板からその長手方向を圧延方向または圧延方向
と直角な方向に一致させて打抜きそのま5、あるいは歪
除去焼鈍後膣扇形素子の継鉄部には扇形のはゾ半径方向
にまた歯部には円周とほぼ平行な方向に所定幅のレーザ
光照射部分が延びかつ該部分が該円周および半径方向に
所定ピッチで配列されるようにパルスレーザ光を照射す
ることを特徴とした大型回転電機固定子の鉄損改善法。1 Each fan-shaped element of the stator core divided into a plurality of pieces is punched from a unidirectional electromagnetic steel sheet with its longitudinal direction aligned with the rolling direction or a direction perpendicular to the rolling direction. A laser beam irradiation part of a predetermined width extends in the radial direction of the fan-shaped yoke part, and a laser beam irradiation part of a predetermined width extends in the tooth part in a direction almost parallel to the circumference, and the parts are arranged at a predetermined pitch in the circumferential and radial direction. A method for improving iron loss in a stator of a large rotating electric machine, which is characterized by irradiating a pulsed laser beam so that the
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP54160502A JPS5937658B2 (en) | 1979-12-11 | 1979-12-11 | Method for improving iron loss in stators of large rotating electric machines |
| GB8033178A GB2062972B (en) | 1979-10-19 | 1980-10-15 | Iron core for electrical machinery and apparatus and well as method for producing the iron core |
| FR8022231A FR2468191A1 (en) | 1979-10-19 | 1980-10-17 | IRON CORE FOR ELECTRICAL MACHINES AND APPARATUS, AND METHOD FOR MANUFACTURING THE CORE |
| DE3039544A DE3039544C2 (en) | 1979-10-19 | 1980-10-20 | Iron core for electrical systems and process for its production |
| US06/615,871 US4613842A (en) | 1979-10-19 | 1984-05-31 | Iron core for electrical machinery and apparatus as well as method for producing the iron core |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP54160502A JPS5937658B2 (en) | 1979-12-11 | 1979-12-11 | Method for improving iron loss in stators of large rotating electric machines |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5683245A JPS5683245A (en) | 1981-07-07 |
| JPS5937658B2 true JPS5937658B2 (en) | 1984-09-11 |
Family
ID=15716319
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP54160502A Expired JPS5937658B2 (en) | 1979-10-19 | 1979-12-11 | Method for improving iron loss in stators of large rotating electric machines |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5937658B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR101195221B1 (en) | 2008-12-03 | 2012-10-29 | 주식회사 포스코 | Iron core of motor with iron loss decreased by magnetic domain refinement and processing method thereof |
-
1979
- 1979-12-11 JP JP54160502A patent/JPS5937658B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5683245A (en) | 1981-07-07 |
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